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Michael Corral: Vector Calculus

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12 CHAPTER 1. VECTORS IN EUCLIDEAN SPACE<br />

Let u=(u 1 ,u 2 ,u 3 ), v=(v 1 ,v 2 ,v 3 ), w=(w 1 ,w 2 ,w 3 ) be vectors in 3 . Then<br />

u+(v+w)=(u 1 ,u 2 ,u 3 )+((v 1 ,v 2 ,v 3 )+(w 1 ,w 2 ,w 3 ))<br />

= (u 1 ,u 2 ,u 3 )+(v 1 +w 1 ,v 2 +w 2 ,v 3 +w 3 ) by Theorem 1.4(b)<br />

= (u 1 +(v 1 +w 1 ),u 2 +(v 2 +w 2 ),u 3 +(v 3 +w 3 )) by Theorem 1.4(b)<br />

= ((u 1 +v 1 )+w 1 ,(u 2 +v 2 )+w 2 ,(u 3 +v 3 )+w 3 ) by properties of real numbers<br />

= (u 1 +v 1 ,u 2 +v 2 ,u 3 +v 3 )+(w 1 ,w 2 ,w 3 ) by Theorem 1.4(b)<br />

= (u+v)+w<br />

This completes the analytic proof of (b). Figure 1.2.6 provides the geometric proof.<br />

u+(v+w)=(u+v)+w<br />

u<br />

u+v<br />

v+w<br />

w<br />

v<br />

Figure 1.2.6 Associative Law for vector addition<br />

(c) We already discussed this on p.10.<br />

(d) We already discussed this on p.10.<br />

(e) We will prove this for a vector v=(v 1 ,v 2 ,v 3 ) in 3 (the proof for 2 is similar):<br />

k(lv)=k(lv 1 ,lv 2 ,lv 3 )<br />

by Theorem 1.4(a)<br />

= (klv 1 ,klv 2 ,klv 3 ) by Theorem 1.4(a)<br />

= (kl)(v 1 ,v 2 ,v 3 ) by Theorem 1.4(a)<br />

= (kl)v<br />

(f) and (g): Left as exercises for the reader.<br />

QED<br />

A unit vector is a vector with magnitude 1. Notice that for any nonzero vector v,<br />

the vector v<br />

1<br />

‖v‖<br />

is a unit vector which points in the same direction as v, since<br />

‖v‖ > 0<br />

and ∥ ∥<br />

v∥<br />

‖v‖<br />

∥= ‖v‖<br />

‖v‖<br />

= 1. Dividing a nonzero vector v by‖v‖ is often called normalizing v.<br />

There are specific unit vectors which we will often use, called the basis vectors:<br />

i=(1,0,0), j=(0,1,0), and k=(0,0,1) in 3 ; i=(1,0) and j=(0,1) in 2 .<br />

These are useful for several reasons: they are mutually perpendicular, since they lie<br />

on distinct coordinate axes; they are all unit vectors:‖i‖=‖j‖=‖k‖=1; every vector<br />

can be written as a unique scalar combination of the basis vectors: v=(a,b)=ai+bj<br />

in 2 , v=(a,b,c)=ai+bj+ck in 3 . See Figure 1.2.7.

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